CN101512854B - Tunable generation of terahertz radiation - Google Patents
Tunable generation of terahertz radiation Download PDFInfo
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- CN101512854B CN101512854B CN2007800325923A CN200780032592A CN101512854B CN 101512854 B CN101512854 B CN 101512854B CN 2007800325923 A CN2007800325923 A CN 2007800325923A CN 200780032592 A CN200780032592 A CN 200780032592A CN 101512854 B CN101512854 B CN 101512854B
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- 230000005855 radiation Effects 0.000 title claims abstract description 61
- 230000005418 spin wave Effects 0.000 claims abstract description 93
- 230000005291 magnetic effect Effects 0.000 claims abstract description 42
- 238000000034 method Methods 0.000 claims abstract description 18
- 230000005684 electric field Effects 0.000 claims description 21
- 230000002706 hydrostatic effect Effects 0.000 claims description 12
- 230000003993 interaction Effects 0.000 claims description 8
- 239000003302 ferromagnetic material Substances 0.000 claims description 7
- 238000005086 pumping Methods 0.000 claims description 4
- 230000000694 effects Effects 0.000 claims description 2
- 239000012530 fluid Substances 0.000 description 10
- 230000003068 static effect Effects 0.000 description 10
- 230000005294 ferromagnetic effect Effects 0.000 description 6
- 239000004065 semiconductor Substances 0.000 description 5
- 230000010287 polarization Effects 0.000 description 4
- 230000008569 process Effects 0.000 description 4
- 230000008859 change Effects 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
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- 230000004048 modification Effects 0.000 description 2
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- 239000012141 concentrate Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000003574 free electron Substances 0.000 description 1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S1/00—Masers, i.e. devices using stimulated emission of electromagnetic radiation in the microwave range
- H01S1/02—Masers, i.e. devices using stimulated emission of electromagnetic radiation in the microwave range solid
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Abstract
A method of tunable generation of terahertz radiation comprising: (A) providing a magnon gain medium; wherein the magnon gain medium supports generation of nonequilibrium magnons; (B) generating terahertz radiation in the magnon gain medium; and (C) tuning frequency of the terahertz radiation by causing changes in an external parameter. The substantial tuning of the frequency of the generated terahertz radiation can be achieved by applying an external magnetic field, and by causing changes in a value of the external magnetic field.
Description
Technical field
The present invention relates to the production method of terahertz (terahertz) ripple.
Background technology
The application numbers of submitting on July 3rd, 2006 is 11/481,197, and the U.S. Patent application that is entitled as " GENERATIONOF TERAHERTZ WAVES " has disclosed the production method of terahertz (THz) radiation.The full text of patent application number 11/481,197 is in this combination and will be called patent application #1 hereinafter.But, the adjustability of the THz ripple of generation then is not discussed.
Summary of the invention
The invention provides a kind of adjustable THz photon production method and device.
One aspect of the present invention relates to a kind of tunable generation of terahertz radiation.
In one embodiment, method of the present invention may further comprise the steps: the magnon gain media (A) is provided; Wherein, the magnon gain media is supported the generation of Nonequilibrium magnetic oscillator; (B) in the magnon gain media, produce terahertz radiation; And, adjust the frequency of terahertz radiation (C) by making changes in external parameters.
In one embodiment of this invention, step (A) further comprises: (A1) the magnon gain media is positioned in the thermostat so that the temperature of magnon gain media remains under the critical temperature.
In one embodiment of this invention, step (A) further comprises: (A2) select the magnon gain media from the group that the following is formed: { ferromagnetic semiconductor; Ferromagnetic insulator; And ferromagnetic material }.In one embodiment of this invention, step (A2) further comprises: (A2,1) will comprise that the magnon gain media of selected ferromagnetic material is positioned in the thermostat so that the temperature of this selected ferromagnetic material remains under its Curie temperature.
In one embodiment of this invention, step (B) further comprises: (B1) nonequilibrium electron is injected the magnon gain media; Wherein, the propagation of nonequilibrium electron in the magnon gain media causes the generation of Nonequilibrium magnetic oscillator; And wherein, the interaction between the Nonequilibrium magnetic oscillator causes the generation of terahertz radiation.In one embodiment of this invention, step (B1) further comprises: (B1,1) pumps into the magnon gain media with nonequilibrium electron.In another embodiment of the present invention, step (B1) further comprises: (B1, the 2) nonequilibrium electron that will polarize pumps into the magnon gain media.In an embodiment more of the present invention, step (B1) further comprises: (B1,3) quantity is enough big polarization nonequilibrium electron pumps into the magnon gain media, and wherein, the polarization nonequilibrium electron that has pumped into that quantity is enough big causes having produced the Nonequilibrium magnetic oscillator in the magnon gain media.In another embodiment of the present invention, step (B1) further comprises: (B1,4) the polarization nonequilibrium electron with number of thresholds pumps into the magnon gain media, and wherein, the polarization nonequilibrium electron of number of thresholds is enough to produce the magnon avalanche effect in the magnon gain media.
In one embodiment of this invention, further comprise by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C1) apply the external magnetic field; And the value of external magnetic field is changed.In this embodiment of the present invention, the frequency of the terahertz radiation of generation changes because of the correlation of the value of the energy of Nonequilibrium magnetic oscillator and external magnetic field.
In another embodiment of the present invention, further comprise by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C3) apply the external fluid static pressure; And the value of external fluid static pressure is changed.In this embodiment of the present invention, the frequency of the terahertz radiation of generation changes because of the stiffness (stiffness) of the Nonequilibrium magnetic oscillator correlation with the value of external fluid static pressure.
In an embodiment more of the present invention, further comprise by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C5) apply external electrical field; And the value of external electrical field is changed.In this embodiment of the present invention, the frequency of the terahertz radiation of generation changes because of the correlation of the value of the stiffness of Nonequilibrium magnetic oscillator and external electrical field.
Another aspect of the present invention relates to a kind of generation device of adjustable terahertz radiation.
In one embodiment, the inventive system comprises: (A) magnon gain media; Wherein, the magnon gain media is supported the generation of Nonequilibrium magnetic oscillator; (B) equipment of generation terahertz radiation in the magnon gain media; And the equipment of (C) adjusting the frequency of the terahertz radiation that is produced.
In one embodiment, device of the present invention further comprises: (D) thermostat.In this embodiment of the present invention, the magnon gain media is positioned in the thermostat, and wherein, is configured to make the temperature of magnon gain media to remain under the critical temperature thermostat.
In one embodiment of this invention, equipment (B) further comprises: the equipment that (B1) nonequilibrium electron is injected the magnon gain media; Wherein the propagation of nonequilibrium electron in the magnon gain media causes the generation of Nonequilibrium magnetic oscillator; And wherein the interaction between the Nonequilibrium magnetic oscillator causes the generation of terahertz radiation.
In one embodiment of this invention, equipment (B1) further comprises: (B1,1) pumps into nonequilibrium electron the equipment of magnon gain media.In another embodiment of the present invention, equipment (B1) further comprises: (B1, the 2) nonequilibrium electron that will polarize pumps into the equipment of magnon gain media.
In one embodiment of this invention, the equipment (C) of the frequency of adjustment terahertz radiation further comprises: the equipment that (C1) applies the external magnetic field; And the equipment that (C2) makes the value change of external magnetic field.
In another embodiment of the present invention, the equipment (C) of adjusting the frequency of terahertz radiation further comprises: the equipment that (C3) applies the external fluid static pressure; And the equipment that (C4) makes the value change of external fluid static pressure.
In an embodiment more of the present invention, the equipment (C) of adjusting the frequency of terahertz radiation further comprises: the equipment that (C5) applies external electrical field; And the equipment that (C6) makes the value change of external electrical field.
Description of drawings
This in conjunction with and the accompanying drawing that constitutes the some of specification embodiments of the invention are shown, and be used to explain principle of the present invention with specification.
Figure 1 shows that to be used for forceful electric power of the present invention-magnon interaction process (comparing) that wherein, the nonequilibrium electron that is excited in the downward last subband of spin is launched the magnon with big wave vector apace with electronics-electronics or electronics-phonon interaction.
Figure 2 shows that the energy that is used for the photon that the present invention launched under the situation of positive adjustability and the relation curve in magnetic field.
Figure 3 shows that the energy that is used for the photon that the present invention launched under the situation of negative adjustability and the relation curve of hydrostatic pressure.
Figure 4 shows that the energy that is used for the photon that the present invention launched under the situation of positive adjustability and the relation curve of carrier concentration.
Embodiment
To mention preferred embodiment of the present invention in detail below, accompanying drawing is depicted as its example.Though hereinafter will narrate the present invention, should be understood that not to be that plan limit the invention to these embodiment in conjunction with preferred embodiment.On the contrary, the present invention is intended to cover spirit and the alternative within the protection range, modification and the equivalent that can be included in as the claims qualification.In addition, having proposed a lot of specific detail in following of the present invention being described in detail, is in order to make the people can understand the present invention up hill and dale.But clearly, for a person skilled in the art, need not these specific detail and all can implement the present invention.In other cases, well-known method, process, parts and circuit are described in detail, in order to avoid unnecessarily fuzzy feature of the present invention.
Below some parts of Xiang Shuing are to represent according to the symbolic notation of particle and quasiparticle interaction, program, equation, branch, chart and other physical process.These narrations and representation are the means by technical staff's employing in this physics field of condensed state matter, so that the main idea of its work is conveyed to most effectively the others skilled in the art in this field.
#1 discloses as patent application, and electronics 20 and spin wave (magnon) 18 interact as shown in Figure 1.Externally the energy of the magnon in the magnetic field H is as follows:
Q herein is the magnon wave vector, and D is the magnon stiffness, and θ is
And magnetic moment
Between angle,
Wherein g is the g factor (g ≈ 2), and μ
BBe Bohr magneton.
The nonequilibrium electron that is excited in downward the last subband (14 among Fig. 1) of spin is promptly launched magnon, moves on to the subband (12 among Fig. 1) that oneself spins up, thereby and then moves on to the bottom ballistic phonon of this subband.
#1 discloses as patent application, and the emission process of magnon is similar to the running of level Four laser system.More particularly, if the nonequilibrium electron of sufficient amount is pumped into downward the last subband of (injection) spin (Fig. 1 14), then the magnon quantity in narrow wave vector scope begins with pumping increase apace.Therefore, this system works as " magnon laser ".
According to the law of conservation of energy and the law of conservation of momentum, if the nonequilibrium electron energy ε that measures from the bottom of the downward subband 14 that spins
pMore much smaller than exchange band gap Δ 16, the wave vector q of the magnon of then being launched 18 is in interval q
1≤ q≤q
2In, wherein
p
0=(2m Δ)
1/2, p=(2m ε
p)
1/2<<p
0, m is an electron effective mass.
At q
1,2Expression formula in, ignored
With
Magnitude (order) light maintenance on the occasion of.Clearance delta is the magnitude of a hundreds of meV.Therefore,
Enough big, so that the Dq in (equation 1)
2The item ratio
Much bigger, and ratio
Much bigger.Here it is, and why we can ignore
The influence that brings with the weak correlation of θ.In this case, (equation 1) can be rewritten as follows:
#1 discloses as patent application, and two merging with magnon of wave vector q and q ' have produced photon, and it has following wave vector
With and frequency v
kBe equal to
ω
q+ ω
q'=v
k=c
k(equation 6)
Wherein c is the light velocity.
According to these laws, k is more much smaller than q, that is to say
Therefore, the frequency of the radiation that is produced is as follows:
Can introduce new parameter, i.e. the adjustability that causes of magnetic field:
According to (equation 8 and 9), t
HFor:
(equation 10)
Therefore, magnetic field H=1T regulates about 6% 1THz radiation frequency.Figure 2 shows that the frequency f of the radiation of generation
rRelation curve 30 with magnetic field H.
As an example, can consider that Curie temperature is T
cThe THz radiation of the ferromagnetic semiconductor EuO of=70K.For EuO, m=0.35m
0, m wherein
0Be the free electron quality, (J.Shoenes and P.Wachter, Phys.Rev.B 9,3097 (1974)), clearance delta=0.6eV (J.Lascaray, J.P.Desfours, and M.Averous, Sol.St.Com.19,677 (1976)), the wave vector of excitation magnon
Spin wave stiffness D=10.810
-16Mevcm
2(L.Passel, O.W.Dietrich and J.Als-Nielsen, Phys.Rev.B14,4897,1976).This has provided the energy of excitation magnon at place, zero magnetic field:
And frequency f
m=ω/2 π ≈ 0.176THz.Therefore, in above-mentioned example, the frequency of the radiation that is produced is: f
r|
H=0=2f
m=0.352THz.
When magnetic field H=1T (tesla), according to (equation 8), the frequency of the radiation of generation is equal to: f
r|
H=1T=0.408THz.So being changed to relatively of the frequency of the radiation that produces: [f
r(H=1T)-f
r(H=0)]/f
r(H=0)=16%.
Also can introduce other three parameters.The adjustability that hydrostatic pressure causes:
The adjustability that carrier concentration causes:
And the adjustability that causes of electric field:
The adjustability t that hydrostatic pressure causes
PCorrelation by stiffness D and hydrostatic pressure P is determined.For example, at T
cThe ferromagnetic semiconductor CdCr of=130K
2Se
4In, T
cReduce with pressure:
See also " Ferromagnetic Materials " (vol.3 is edited by E.P.Wolfarth, North-Holland Publishing Company, 1982) of R.P.Van Stapele.T
cVariation relate to the correlation of exchange integral and lattice constant.Can expect that the correlation of D and P is similar to T
cCorrelation with P.So, radiation frequency f
rDepend on P (50 among Fig. 3).
In ferromagnetic semiconductor, stiffness D also can be depending on carrier concentration n
cIf-RKKY (Ruderman-Kittel-Kasuya-Yosida) indirect exchange has very crucial contribution to D.If this kind situation, the adjustability T that carrier concentration causes
c(equation 12) is by D and n
cCorrelation determine.Figure 4 shows that the frequency f of the radiation of generation
rWith carrier concentration n
cRelation curve 60.
Some situation also, carrier concentration n
cAnd stiffness D depends on external electrical field E.In these cases, can utilize the electric field that meets equation 13 to adjust the frequency of generation.
In one embodiment, adjustable generation of terahertz radiation of the present invention comprises (not shown): the magnon gain media (A) is provided; Wherein the magnon gain media is supported the generation of Nonequilibrium magnetic oscillator; (B) in the magnon gain media, produce terahertz radiation; And (C) by making changes in external parameters adjust the frequency of terahertz radiation.
Patent application #1 has intactly disclosed two steps (A) and (B).So this paper will concentrate on step (C): adjust the frequency of terahertz radiation by making changes in external parameters.
In one embodiment of this invention, the frequency of the terahertz radiation of generation changes because of the energy of Nonequilibrium magnetic oscillator and the correlation of external magnetic field value.See also (equation 9) and (equation 10).In this embodiment of the present invention, comprise (not shown) by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C1) device of the present invention is applied external magnetic field (#1 discloses as patent application); And the value of external magnetic field is changed.The basic structure of device of the present invention (#1 discloses as patent application) comprising: (A) magnon gain media (for example ferromagnetic semiconductor); (B) nonequilibrium electron source; And (C) be configured to temperature with the magnon gain media and remain on thermostat under the critical temperature.For a person skilled in the art, how to apply external magnetic field and the value of the external magnetic field that is applied is changed is well-known.
In another embodiment of the present invention, the frequency of the terahertz radiation of generation changes because of the correlation of the value of the stiffness of Nonequilibrium magnetic oscillator and external fluid static pressure.See also (equation 11).In this embodiment of the present invention, further comprise by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C3) device of the present invention is applied external fluid static pressure (#1 discloses as patent application); And the value of external fluid static pressure is changed.For a person skilled in the art, how to apply external fluid static pressure and the value of the external fluid static pressure that is applied is changed is well-known.
In an embodiment more of the present invention, the frequency of the terahertz radiation of generation changes because of the correlation of the value of the stiffness of Nonequilibrium magnetic oscillator and external electrical field.See also (equation 13).In this embodiment of the present invention, further comprise by making changes in external parameters adjust the step of the frequency of terahertz radiation (C): (C5) device of the present invention is applied external electrical field (#1 discloses as patent application); And the value of external electrical field is changed.For a person skilled in the art, how to apply external electrical field and the value of the external electrical field that is applied is changed is well-known.
For the purpose that illustrates and narrate, specific embodiment of the present invention has been shown above.They do not plan to be used as exhaustive or limit the invention to shown in definite form really, clearly,, can make a lot of remodeling and modification according to above-mentioned enlightenment.Select and narration embodiment is for principle of the present invention and actual application thereof can be described best, thereby make others skilled in the art can utilize the present invention and different embodiment best by the improvement of the various special-purposes that are suitable for expecting.Protection scope of the present invention should be limited by appended claim and their equivalent.
Claims (18)
Applications Claiming Priority (3)
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US11/496,889 US7440178B2 (en) | 2006-07-03 | 2006-07-31 | Tunable generation of terahertz radiation |
US11/496,889 | 2006-07-31 | ||
PCT/US2007/067272 WO2008016731A2 (en) | 2006-07-31 | 2007-04-24 | Tunable generation of terahertz radiation |
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CN101512854B true CN101512854B (en) | 2011-05-04 |
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US8084374B2 (en) * | 2009-11-19 | 2011-12-27 | Washington University In St. Louis | Tuning of photo-absorption materials through use of magnetic fields |
US9551619B1 (en) | 2011-09-23 | 2017-01-24 | Rockwell Collins, Inc. | Terahertz laser |
US9764208B1 (en) * | 2016-05-31 | 2017-09-19 | Parsons Xtreme Golf, LLC | Golf club heads and methods to manufacture golf club heads |
US20170368429A1 (en) * | 2014-02-20 | 2017-12-28 | Parsons Xtreme Golf, LLC | Golf club heads and methods to manufacture golf club heads |
US20180236323A9 (en) * | 2014-02-20 | 2018-08-23 | Parsons Xtreme Golf, LLC | Golf club heads and methods to manufacture golf club heads |
US20180236325A1 (en) * | 2014-02-20 | 2018-08-23 | Parsons Xtreme Golf, LLC | Golf club heads and methods to manufacture golf club heads |
US20180221727A1 (en) * | 2014-02-20 | 2018-08-09 | Parsons Xtreme Golf, LLC | Golf club heads and methods to manufacture golf club heads |
CN108023263B (en) * | 2017-11-20 | 2020-03-10 | 中国工程物理研究院电子工程研究所 | Terahertz pulse generator for regulating and controlling magnetic field and voltage |
US10892602B1 (en) * | 2019-01-10 | 2021-01-12 | Magtera, Inc. | Tunable multilayer terahertz magnon generator |
CN113519098A (en) * | 2019-01-10 | 2021-10-19 | 玛格特拉公司 | Coherent terahertz magnon lasers and coherent terahertz communication systems |
Citations (2)
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US3986194A (en) * | 1974-08-15 | 1976-10-12 | National Research Institute For Metals | Magnetic semiconductor device |
CN1639929A (en) * | 2002-02-28 | 2005-07-13 | 费姆托激光产品股份有限公司 | Device for generating terahertz radiation, and a semiconductor component |
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US7430074B2 (en) * | 2006-07-03 | 2008-09-30 | Terahertz Technologies, Llc | Generation of Terahertz waves |
-
2006
- 2006-07-31 US US11/496,889 patent/US7440178B2/en active Active
-
2007
- 2007-04-24 EP EP07761170.5A patent/EP2047572B1/en not_active Not-in-force
- 2007-04-24 WO PCT/US2007/067272 patent/WO2008016731A2/en active Search and Examination
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Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3986194A (en) * | 1974-08-15 | 1976-10-12 | National Research Institute For Metals | Magnetic semiconductor device |
CN1639929A (en) * | 2002-02-28 | 2005-07-13 | 费姆托激光产品股份有限公司 | Device for generating terahertz radiation, and a semiconductor component |
Non-Patent Citations (8)
Title |
---|
Korenblit et al..Generation of high-frequency magnons in a ferromagnetic semiconductor.《JETP Letters》.1976,vol.24(no.11),556-558. * |
Korenblit et al..high frequency magnon generation by nonequilibrium electrons and the instability of the magnon system.《PHYSICS LETTERS》.1977,vol.64a(no.3),307-308. * |
Korenblitetal..Generationofhigh-frequencymagnonsinaferromagneticsemiconductor.《JETPLetters》.1976 vol.24(no.11) |
Korenblitetal..highfrequencymagnongenerationbynonequilibriumelectronsandtheinstabilityofthemagnonsystem.《PHYSICSLETTERS》.1977 vol.64a(no.3) |
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US7440178B2 (en) | 2008-10-21 |
EP2047572B1 (en) | 2018-02-21 |
EP2047572A2 (en) | 2009-04-15 |
EP2047572A4 (en) | 2013-07-17 |
WO2008016731A3 (en) | 2008-12-24 |
CN101512854A (en) | 2009-08-19 |
WO2008016731A2 (en) | 2008-02-07 |
US20080002250A1 (en) | 2008-01-03 |
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